TWI430576B - System for improved phase noise in a bicmos clock driver - Google Patents
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- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
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- H03K3/00—Circuits for generating electric pulses; Monostable, bistable or multistable circuits
- H03K3/02—Generators characterised by the type of circuit or by the means used for producing pulses
- H03K3/353—Generators characterised by the type of circuit or by the means used for producing pulses by the use, as active elements, of field-effect transistors with internal or external positive feedback
- H03K3/356—Bistable circuits
- H03K3/356104—Bistable circuits using complementary field-effect transistors
- H03K3/356113—Bistable circuits using complementary field-effect transistors using additional transistors in the input circuit
- H03K3/35613—Bistable circuits using complementary field-effect transistors using additional transistors in the input circuit the input circuit having a differential configuration
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- H—ELECTRICITY
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- H03K19/00—Logic circuits, i.e. having at least two inputs acting on one output; Inverting circuits
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- H—ELECTRICITY
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- H03K19/00—Logic circuits, i.e. having at least two inputs acting on one output; Inverting circuits
- H03K19/01—Modifications for accelerating switching
- H03K19/017—Modifications for accelerating switching in field-effect transistor circuits
- H03K19/01707—Modifications for accelerating switching in field-effect transistor circuits in asynchronous circuits
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- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03K—PULSE TECHNIQUE
- H03K19/00—Logic circuits, i.e. having at least two inputs acting on one output; Inverting circuits
- H03K19/0175—Coupling arrangements; Interface arrangements
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- H03K19/017518—Interface arrangements using a combination of bipolar and field effect transistors [BIFET]
- H03K19/017527—Interface arrangements using a combination of bipolar and field effect transistors [BIFET] with at least one differential stage
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- H—ELECTRICITY
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- H03K3/00—Circuits for generating electric pulses; Monostable, bistable or multistable circuits
- H03K3/01—Details
- H03K3/013—Modifications of generator to prevent operation by noise or interference
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- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03K—PULSE TECHNIQUE
- H03K3/00—Circuits for generating electric pulses; Monostable, bistable or multistable circuits
- H03K3/02—Generators characterised by the type of circuit or by the means used for producing pulses
- H03K3/021—Generators characterised by the type of circuit or by the means used for producing pulses by the use, as active elements, of more than one type of element or means, e.g. BIMOS, composite devices such as IGBT
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Description
本發明係關於一種用於時脈驅動器之方法及系統,及使用該方法及系統之多個系統。更特定言之,本發明係關於一種用於BiCMOS時脈驅動器之方法及系統,及使用該方法及系統之多個系統。The present invention relates to a method and system for a clock driver, and a plurality of systems using the method and system. More particularly, the present invention relates to a method and system for a BiCMOS clock driver, and a plurality of systems using the method and system.
現今之訊號處理系統經常要對具有寬動態範圍的高速訊號進行數位化及處理。數位化包括:將一訊號量化(quantize)成離散級,例如以n位元類比至數位轉換器(ADC)量化成2n 等級;及以離散時間間隔對一訊號進行取樣。某些高速輸入訊號之頻率係高於所使用的ADC之取樣率,如此造成所謂的「低取樣」,此時需要藉助精確的重複參考時間。否則,取樣操作的時間不確定性可能產生比量化程序時還大的誤差。此一熟知的問題記載於美國專利編號US7,345,528(發明名稱“Method and Apparatus for Improved Clock PreAmplifier with Low Jitter”,後稱「’528專利」)說明書之「先前技術」段落。Today's signal processing systems often digitize and process high-speed signals with a wide dynamic range. Digitization includes quantifying a signal into discrete levels, such as an n-bit analog to digital converter (ADC) quantized to a 2 n level; and sampling a signal at discrete time intervals. The frequency of some high-speed input signals is higher than the sampling rate of the ADC used, which causes so-called "low sampling", which requires accurate repeat reference time. Otherwise, the time uncertainty of the sampling operation may result in a larger error than when the quantization procedure was performed. This well-known problem is described in the "Prior Art" section of U.S. Patent No. 7,345,528, entitled "Method and Apparatus for Improved Clock Pre-Amplifier with Low Jitter" (hereinafter referred to as "the '528 patent").
用於此一系統的理想的時脈訊號係一具有完美固定週期的重複波形。每一單一週期應具有與其它週期完全相同的期間。實際時脈訊號相對於每一週期期間之波動可特徵化為跳動(jitter)(在時間域中)或相位雜訊(在頻率域中)。在某些假設下,後者可被轉換成前者。一般會希望跳動或相位雜訊能儘可能的小。The ideal clock signal for this system is a repetitive waveform with a perfect fixed period. Each single cycle should have exactly the same period as the other cycles. The actual clock signal can be characterized as jitter (in the time domain) or phase noise (in the frequency domain) with respect to fluctuations during each cycle. Under certain assumptions, the latter can be converted into the former. It is generally expected that the jitter or phase noise can be as small as possible.
為了達成低相位雜訊之目的,已進行各種不同嘗試。例如,可將低雜訊的雙載子接面電晶體(BJT,Bipolar Junction Transistor)電路製作成(例如)射極耦接邏輯形式(ECL,Emitter-Coupled Logic),以達到足夠低的相位雜訊。BJT電路保留了訊號速度及低振幅的雜訊整體性。Various attempts have been made to achieve low phase noise. For example, a low-noise bipolar junction transistor (BJT) circuit can be fabricated, for example, in an emitter-coupled logic form (ECL, Emitter-Coupled Logic) to achieve a sufficiently low phase miscellaneous News. The BJT circuit preserves signal speed and low amplitude noise integrity.
雖然在MOSFET裝置本身存在較高雜訊,習知的CMOS邏輯電路亦可用來達成低相位雜訊目的,因為邏輯擺動會較大(軌對軌)而相位雜訊具有訊號對雜訊(Signal-to-Noise)特性。亦即,較大的雜訊可藉由使用較高的軌對軌訊號位準來克服。Although there is high noise in the MOSFET device itself, the conventional CMOS logic circuit can also be used to achieve low phase noise because the logic swing is large (rail-to-rail) and the phase noise has signal-to-noise (Signal- to-Noise) feature. That is, larger noise can be overcome by using a higher rail-to-rail signal level.
僅當可獲得一軌對軌訊號擺動時,CMOS可同時保留速度及雜訊。然而,低相位雜訊訊號之各種訊號源幾乎無法傳送真實的軌對軌CMOS邏輯位準,不論訊號源係石英晶體振盪器、共振振盪器或透過一媒體傳送訊號之載體。因此,當欲將一低相位雜訊訊號由低位準(諸如ECL或一小正弦波形)轉譯成CMOS邏輯位準時會產生問題。CMOS can retain both speed and noise only when a track-to-rail signal swing is available. However, various sources of low-phase noise signals are almost incapable of transmitting true rail-to-rail CMOS logic levels, regardless of whether the signal source is a quartz crystal oscillator, a resonant oscillator, or a carrier that transmits signals through a medium. Therefore, problems arise when a low phase noise signal is to be translated from a low level (such as an ECL or a small sinusoidal waveform) into a CMOS logic level.
存在各種習知解決方案來克服將一低相位雜訊訊號由低位準轉譯成CMOS邏輯位準時所產生之問題。不幸的是,這些習知的解決手段一般會造成不良的相位雜訊、速度限制、或過度耗損電源三者中之一或多種問題。例如,美國專利編號US5,019,726(發明名稱“BiCMOS ECL-TO-CMOS Conversion Circuit”,後稱「’726專利」)揭示一種轉換電路,其於輸入端由差動ECL訊號及三個MOSFET閘所構成的電路負載來驅動。’726專利中之MOSFET閘之電容性負載不是會限制電路之操作速度,就是需要大量電源供應來驅動該等閘。依實現方式之不同,’726專利所建議的解決方案可能會提高雜訊位準。此外,上方BJT之基極節點於每一週期會有一大的電壓擺動通過。因此,當與必然存在的轉換率(slew rate)限制共同作用時,會產生時序不確定性。當用於對該基極節點之電容充電之電流(由上方PMOS或最下方NMOS決定)有雜訊時,相位雜訊會基於雜訊位準而成比例地降級。要產生一由一閒置狀態到達一交換點的電壓擺動所需之時間係與轉換率成反比。There are various conventional solutions to overcome the problems associated with translating a low phase noise signal from a low level to a CMOS logic level. Unfortunately, these conventional solutions typically result in one or more of poor phase noise, speed limitations, or excessive power loss. For example, U.S. Patent No. 5,019,726, entitled "BiCMOS ECL-TO-CMOS Conversion Circuit" (hereinafter referred to as "the '726 patent") discloses a conversion circuit having a differential ECL signal and three MOSFET gates at the input end. The constructed circuit load is driven. The capacitive loading of the MOSFET gates of the '726 patent does not limit the operating speed of the circuit, or requires a large amount of power supply to drive the gates. Depending on the implementation, the solution proposed by the '726 patent may increase the level of noise. In addition, the base node of the upper BJT will have a large voltage swing through each cycle. Therefore, timing uncertainty occurs when combined with the inevitable slew rate limit. When there is noise in the current used to charge the capacitor of the base node (determined by the upper PMOS or the lowest NMOS), the phase noise is proportionally degraded based on the noise level. The time required to generate a voltage swing from an idle state to an exchange point is inversely proportional to the slew rate.
美國專利編號US5,631,580(發明名稱「BiCMOS ECL-to-CMOS Level Converter」,後稱「’580專利」)揭示另一先前技術之解決方案,其中存在低位準訊號擺動,直到一軌對軌CMOS訊號產生為止。然而,所揭示之電路之效能仍然無法產生所要的相位雜訊表現,因為由PMOSFET(其閘極與汲極相連接)所造成的雜訊位準仍然太高。這限制了可用的電壓擺動,而因此使訊雜比降級。即便沒有此限制,當互補式輸出BJT關閉時,其基極被驅動遠至其射極、至電源軌。這表示存在一訊號擺動,其由一閒置狀態至交換點之擺動為數百毫伏特(在-55℃下高達900mV)。雖然’580專利相對於’726專利進行了改良,然而因為雜訊仍然太大,而由於電流雜訊及所發生的轉換率限制,進而導致相位雜訊之表現下降。U.S. Patent No. 5,631,580, entitled "BiCMOS ECL-to-CMOS Level Converter", hereinafter referred to as "the '580 patent", discloses another prior art solution in which there is a low level signal swing until a rail-to-rail CMOS The signal is generated. However, the performance of the disclosed circuit still does not produce the desired phase noise performance because the noise level caused by the PMOSFET (whose gate is connected to the drain) is still too high. This limits the available voltage swing and thus degrades the signal to noise ratio. Even without this limitation, when the complementary output BJT is turned off, its base is driven as far as its emitter to the power rail. This means that there is a signal swing that swings from an idle state to the switching point to hundreds of millivolts (up to 900 mV at -55 °C). Although the '580 patent has been improved over the '726 patent, the noise is still too large, and the performance of the phase noise is degraded due to current noise and the conversion rate limitation.
在美國專利編號US5,900,746中(發明名稱「Ultra Low Jitter Differential to Fullswing BiCMOS Comparator with equal rise/fall time and Complementary Outputs」,後稱「’746專利」),藉由使用一虛擬反相器來將第一CMOS閘之輸入保持在靠近交換臨界點之一靜態位準,且動態驅動訊號係一來自BJT差動對之低位準訊號。因此,具有要轉換的重大電壓變化的第一節點為第一軌對軌CMOS訊號。然而,驅動第一MOSFET之閘極之訊號本質為電流驅動訊號。因此,邊緣之轉換率係由驅動電路中之靜態電流位準及從反相器之MOSFET閘極看進去之電容來決定。該等電容包括閘至源極電容、閘至主體(bulk)電容及閘至汲極電容。因此,閘至汲極電容會因熟知的米勒效應而被放大數倍,由於連接至汲極之相反薄板而提升了有效電容。亦即,反相器輸出具有一大的相反電壓擺動。U.S. Patent No. 5,900,746 (Ultra Low Jitter Differential to Fullswing BiCMOS Comparator with equal rise/fall time and Complementary Outputs, hereinafter referred to as '746 patent), by using a virtual inverter The input of the first CMOS gate is maintained at a static level close to one of the switching thresholds, and the dynamic driving signal is a low level signal from the BJT differential pair. Therefore, the first node having a significant voltage change to be converted is the first rail-to-rail CMOS signal. However, the signal driving the gate of the first MOSFET is essentially a current drive signal. Therefore, the edge conversion rate is determined by the quiescent current level in the driver circuit and the capacitance seen from the MOSFET gate of the inverter. These capacitors include gate-to-source capacitance, gate-to-bulk capacitance, and gate-to-drain capacitance. Therefore, the gate-to-drain capacitance is amplified several times due to the well-known Miller effect, which increases the effective capacitance due to the opposite thin plate connected to the drain. That is, the inverter output has a large opposite voltage swing.
以這種電流源來驅動閘極可能產生可接受的速度,但由於出現在電流源上的雜訊,常使得雜訊表現不好。通常係以習知的參考帶隙類型產生晶載(on-chip)電流源,以提供幾乎不受供應電壓及溫度影響的電流,或與絕對溫度成正比的電流。雖然’746專利中所揭示的電路在某些情況下提供了某些所需特性,然而基於參考帶隙的電流源的動態範圍(其係定義為由電流雜訊位準區隔開的靜態電流位準)常會造成限制而無法達成最需要的相位雜訊表現。Driving the gate with this current source may produce acceptable speeds, but due to the noise present on the current source, the noise often does not perform well. An on-chip current source is typically generated with conventional reference bandgap types to provide a current that is substantially unaffected by supply voltage and temperature, or a current that is proportional to absolute temperature. Although the circuit disclosed in the '746 patent provides certain desirable characteristics in some cases, the dynamic range of the current source based on the reference bandgap is defined as the quiescent current separated by the current noise leveling region. Levels often cause limitations and do not achieve the most needed phase noise performance.
美國專利編號US6,008,667(發明名稱「Emitter-Coupled Logic to CMOS Logic Converter and method of operation」,後稱「’667」專利)揭示了另一先前技術電路。在’667專利所描述的電路中,產生第一軌對軌CMOS訊號之NMOS及PMOS電晶體之閘極,係獨立地以一小電壓擺動來驅動,該電壓擺動係以每一個別MOSFET之臨限Vgs為中心進行擺動。如此可改善一特定位準之靜態電流汲極之速度,其由測量閘驅動訊號之傳送延遲及轉換率二者來獲得。反相器MOSFET之雜訊來源之一者為輸入參考電壓雜訊。因此,轉換率(每秒伏特)愈快,愈少電壓雜訊被轉換成相位雜訊。Another prior art circuit is disclosed in U.S. Patent No. 6,008,667, entitled "Emitter-Coupled Logic to CMOS Logic Converter and method of operation" (hereinafter referred to as "the '667" patent). In the circuit described in the '667 patent, the gates of the NMOS and PMOS transistors that generate the first rail-to-rail CMOS signal are independently driven by a small voltage swing, which is followed by each individual MOSFET. The Vgs are limited to swing at the center. This improves the speed of a particular level of quiescent current drain, which is obtained by measuring both the transfer delay and the slew rate of the gate drive signal. One of the sources of noise for the inverter MOSFET is the input reference voltage noise. Therefore, the faster the conversion rate (volts per second), the less the voltage noise is converted into phase noise.
然而,‘667專利所揭示的電路亦具有二缺點,此二缺點亦出現在其它先前技術電路中。第一缺點為,閘驅動訊號仍然係由該級之靜態電流所限制。反相器閘節點處之閘極與汲極相連接的MOSFET企圖降低阻抗,使該驅動器更類似一電壓源。因此這樣的MOSFET,作為被動元件,不會增加可用來驅動反相器閘極端之電流。第二缺點為,這些MOSFET的閘極與汲極相連接,本身會限制訊雜比,已如前述。However, the circuit disclosed in the '667 patent also has two drawbacks, which are also present in other prior art circuits. The first drawback is that the gate drive signal is still limited by the quiescent current of the stage. The MOSFET whose gate is connected to the drain at the gate of the inverter attempts to reduce the impedance, making the driver more similar to a voltage source. Therefore, such a MOSFET, as a passive component, does not increase the current available to drive the inverter gate terminal. The second disadvantage is that the gates of these MOSFETs are connected to the drain and limit the signal-to-noise ratio itself, as described above.
美國專利編號US7,345,528(後稱「’528專利」)所揭示之電路使用一共用節點來驅動第一反相器之閘極,該共用節點係保持在電源供應位準之適當中間位準(亦見’746專利所揭示之電路)。在’528專利中,驅動器電路包括互補式差動BJT對,以改善在一特定靜態電流位準下之訊雜比。’528專利所揭示之電路以訊號驅動具有高阻抗之反相器輸入,但藉由改變驅動該些節點的電流槽及電流源來改善訊雜比,且改善幅度達兩倍。此外,’528專利揭示一雙極箍位電路,其限制反相器輸入處之電壓擺動,其可改善相位雜訊表現,已如前述。The circuit disclosed in U.S. Patent No. 7,345,528 (hereinafter referred to as "the '528 patent") uses a common node to drive the gate of the first inverter, which maintains an appropriate intermediate level at the power supply level ( See also the circuit disclosed in the '746 patent. In the '528 patent, the driver circuit includes complementary differential BJT pairs to improve the signal to noise ratio at a particular quiescent current level. The circuit disclosed in the '528 patent uses a signal to drive an inverter input having a high impedance, but improves the signal-to-noise ratio by varying the current slots and current sources driving the nodes, and the amplitude is improved by a factor of two. In addition, the '528 patent discloses a bipolar pinch circuit that limits the voltage swing at the input of the inverter, which improves phase noise performance as previously described.
第1圖(先前技術)圖示另一先前技術電路,用以由一習知ECL邏輯閘(包括電晶體115及120)驅動一P-MOSFET對(150及155)之閘極端。當此電路係以積體電路製程製作並合理控制一NPN電晶體之Vbe位準及一PMOS電晶體(150及155)之臨界位準Vgs的情況下,可將此電路依據本領域所熟習之技術製作成在各種操作溫度下具有適當的電壓擺動設定,以執行正確功能。此電路之輸入為ECL邏輯訊號,而其輸出係用來產生CMOS邏輯訊號,下文將進一步說明之。Figure 1 (Prior Art) illustrates another prior art circuit for driving the gate terminals of a pair of P-MOSFETs (150 and 155) by a conventional ECL logic gate (including transistors 115 and 120). When the circuit is fabricated in an integrated circuit process and the Vbe level of an NPN transistor and the critical level Vgs of a PMOS transistor (150 and 155) are properly controlled, the circuit can be used in accordance with the art. The technology is fabricated with appropriate voltage swing settings at various operating temperatures to perform the correct function. The input to this circuit is the ECL logic signal, and its output is used to generate CMOS logic signals, as explained further below.
如第1圖所示之數位邏輯電路僅具有二個靜態,二靜態間之轉換(希望能夠)以快速動態方式進行。當輸入狀態改變時,二PMOS裝置中之一者(例如,150)被連接至其閘極之NPN射極隨耦器(例如,130)關閉。這通常發生相當快且伴隨小的雜訊,因為NPN射極隨耦器(例如,130)作用如一電壓源,其由於裝置之電流增益而隨著其基極端之訊號來增加將節點上拉所需的電流。然而,在另一半的電路中,其它的PMOS裝置(例如,155)將開啟,但這不會那麼快地發生,因為射極隨耦器(例如,135)會截止(掉至零射極電流),除非射極隨耦器之靜態偏壓電流(145)係設定在非常高的位準。如前所述,從MOSFET之閘極看進去的電容包括閘至源極電容、閘至主體電容及閘至汲極電容,其中閘至汲極電容會因熟知的米勒效應而被乘上數倍。The digital logic circuit shown in Figure 1 has only two static, two static transitions (hopefully) can be performed in a fast dynamic manner. When the input state changes, one of the two PMOS devices (eg, 150) is turned off by the NPN emitter follower (eg, 130) connected to its gate. This usually occurs fairly quickly with small noise, because the NPN emitter follower (eg, 130) acts as a voltage source that increases the node's current gain and increases with its base extremes. The current required. However, in the other half of the circuit, the other PMOS devices (eg, 155) will turn on, but this will not happen so quickly because the emitter follower (eg, 135) will turn off (fall to zero emitter current) ), unless the static bias current (145) of the emitter follower is set at a very high level. As mentioned earlier, the capacitance seen from the gate of the MOSFET includes the gate-to-source capacitance, the gate-to-body capacitance, and the gate-to-drain capacitance, where the gate-to-drain capacitance is multiplied by the well-known Miller effect. Times.
在ECL邏輯閘能產生這樣的數倍的電容及快速轉換率下,需要大量的靜態電流來使NPN射極隨耦器(例如,135)在訊號之下降邊緣期間被主動偏壓。此大的偏壓位準將造成通常不希望造成的所有結果,包括增加供應電軌功率消耗及晶片上增加熱產生。亦會造成電路的雜訊增加,因為NPN基極電流雜訊會作用於上拉電阻R4(110),其係比互導(gm)的倒數還要大得多。亦即,基極端之電壓雜訊位準並不是由一般的電壓雜訊項所決定,而是由電流雜訊與上拉電阻之值二者相乘來決定。At ECL logic gates capable of producing such multiples of capacitance and fast slew rate, a large amount of quiescent current is required to cause the NPN emitter follower (e.g., 135) to be actively biased during the falling edge of the signal. This large bias level will result in all undesirable results, including increased supply rail power consumption and increased heat generation on the wafer. This also increases the noise of the circuit because the NPN base current noise acts on the pull-up resistor R4 (110), which is much larger than the reciprocal of the mutual conductance (gm). That is, the voltage noise level of the base terminal is not determined by the general voltage noise term, but by the multiplication of the current noise and the value of the pull-up resistor.
在一典型的靜態電流位準下,雜訊在一可接受程度下維持在用於關閉PMOS裝置之訊號邊緣上。然而,時基雜訊主要係由用於開啟PMOS裝置之訊號邊緣上的電流源的雜訊來決定。At a typical quiescent current level, the noise is maintained at an acceptable level on the edge of the signal used to turn off the PMOS device. However, time-based noise is primarily determined by the noise used to turn on the current source on the edge of the signal of the PMOS device.
第1圖之先前技術的另一方案為將電晶體Q5及Q6改變成N通道MOSFET。這些源極隨耦器與前述射極隨耦器作用相同,二者在功能上皆屬電壓隨耦器之一類。使用NMOS會引入與Vgs(on) 變化性相關的問題,特別是由於主體效應而使得Vgs(on) 會隨著主體電壓而變。然而使用射極隨耦器時主要的雜訊項─基極電流脈衝雜訊─會消失,這是由於MOSFET之閘極電流雜訊大小小數個等級所致。因此在使用NMOS型的電壓隨耦器的情況下,可能可增加來自I2及I3的電流,但不會產生像使用NPN型電壓隨耦器一樣大的雜訊負擔。Another solution of the prior art of Figure 1 is to change transistors Q5 and Q6 to N-channel MOSFETs. These source followers are identical to the aforementioned emitter followers, both of which are functionally a class of voltage followers. The use of NMOS introduces problems associated with Vgs (on) variability, especially due to the subject effect such that Vgs (on) will vary with the subject voltage. However, the main noise term when using the emitter follower - the base current pulse noise - will disappear due to the fractional level of the gate current noise of the MOSFET. Therefore, in the case of using an NMOS type voltage follower, it is possible to increase the current from I2 and I3, but it does not generate a noise load as large as the NPN type voltage follower.
第2圖(先前技術)圖示先前技術解決手段200以產生習知CMOS邏輯訊號,以用於第1圖所示之電路。在電路200中,反平行CMOS反相器230及240係設置於PMOS電晶體210及220之汲極上以形成一鎖存器(latch),其配合第1圖之電路100在二邏輯狀態間進行設定及重置。這適合實現於包括NPN BJT而非PNP BJT的CMOS製程中。然而,電路200將導致二輸出處的工作週期的輕微偏斜(skew)。PMOS裝置210及220中之一者一般關閉速度較其對應PMOS的開啟速度快,如前參照第1圖所述。就第2圖所示的電路200中的競爭觀點而言,這是想要的。然而,由於每一輸出的上升邊緣係由PMOS裝置主動拉起,而下降邊緣會落後大概一個反相器延遲時間,因此偏斜會發生在輸出端。如此一來,第2圖所示的二輸出的工作週期將會偏斜,因此相較於ECL輸出,在一週期內的高能狀態會比低能狀態稍微長些。Figure 2 (Prior Art) illustrates prior art means 200 for generating conventional CMOS logic signals for use in the circuit shown in Figure 1. In circuit 200, anti-parallel CMOS inverters 230 and 240 are disposed on the drains of PMOS transistors 210 and 220 to form a latch that cooperates with circuit 100 of FIG. 1 between two logic states. Set and reset. This is suitable for implementation in CMOS processes including NPN BJT rather than PNP BJT. However, circuit 200 will result in a slight skew of the duty cycle at the two outputs. One of the PMOS devices 210 and 220 generally has a faster turn-off speed than its corresponding PMOS turn-on speed, as previously described with reference to FIG. This is desirable in terms of the competition in the circuit 200 shown in Fig. 2. However, since the rising edge of each output is actively pulled up by the PMOS device and the falling edge is behind about one inverter delay time, the skew occurs at the output. As a result, the duty cycle of the two outputs shown in Figure 2 will be skewed, so the high energy state in one cycle will be slightly longer than the low energy state compared to the ECL output.
第3圖(先前技術)圖示第1圖之電路100的一全差動與互補式實現方式300。一互補式電路係為本領域技藝人士所熟知的,且其中以鏡像方式覆加一第二電路。所有BJT之極性皆從NPN翻轉為PNP,反之亦然;而所有MOSFET之極性皆從PMOS翻轉為NMOS,反之亦然。一般而言,在二供應軌間以中置點為準之鏡像關係下,訊號及偏壓電壓會有相等大小,但會具有相反極性。電路300可僅以包括NPN、PNP BJT及CMOS裝置之製程來實現。這樣的製程係製作互補式電路所需的,且常用於高速、低雜訊電路中。在第3圖中,輸入電晶體310及315係連接至二PNP電壓隨耦器360及375,該等PNP電壓隨耦器進一步驅動二N-MOSFET電晶體385及390之閘極端。此外,互補側包括二輸入電晶體320及325,其係連接至二NPN電壓隨耦器345及365,該等NPN電壓隨耦器驅動二P-MOSFET電晶體377及380之閘極端。Figure 3 (Prior Art) illustrates a fully differential and complementary implementation 300 of circuit 100 of Figure 1. A complementary circuit is well known to those skilled in the art, and wherein a second circuit is mirrored. The polarity of all BJTs is flipped from NPN to PNP, and vice versa; and the polarity of all MOSFETs is flipped from PMOS to NMOS and vice versa. In general, in the mirror relationship between the two supply rails with the neutral point as the standard, the signal and the bias voltage will be equal in size, but will have opposite polarities. Circuit 300 can be implemented only in a process that includes NPN, PNP BJT, and CMOS devices. Such processes are required for making complementary circuits and are commonly used in high speed, low noise circuits. In FIG. 3, input transistors 310 and 315 are coupled to two PNP voltage followers 360 and 375 which further drive the gate terminals of the two N-MOSFET transistors 385 and 390. In addition, the complementary side includes two input transistors 320 and 325 that are coupled to two NPN voltage followers 345 and 365 that drive the gate terminals of the two P-MOSFET transistors 377 and 380.
四個電壓隨耦器(345、365、360及375)驅動四個MOSFET(377、380、385及390),以於輸出端產生第一CMOS軌對軌邏輯訊號。鎖存器電路不需要與第2圖所示之電路200類似。由於電路300僅僅是第1圖之互補版本,因此其在MOSFET閘之驅動方面具有相同特性與缺點。亦即,射極隨耦器作用為電壓源而閘會快速地驅動至關閉狀態。閘驅動至開啟狀態會有電流限制,因此速度會較慢驅動至開啟狀態且亦受較多雜訊干擾,除非靜態電流源大大增加。在該情況下,雜訊位準無論如何會因基極電流雜訊(其流經電阻而引起基極節點上之雜訊)而上升。Four voltage followers (345, 365, 360, and 375) drive four MOSFETs (377, 380, 385, and 390) to produce a first CMOS rail-to-rail logic signal at the output. The latch circuit need not be similar to the circuit 200 shown in FIG. Since circuit 300 is merely a complementary version of Figure 1, it has the same characteristics and disadvantages in driving the MOSFET gate. That is, the emitter follower acts as a voltage source and the gate is quickly driven to the off state. There is a current limit when the gate is driven to the on state, so the speed will be driven slower to the on state and also subject to more noise, unless the quiescent current source is greatly increased. In this case, the noise level rises anyway due to base current noise, which causes noise on the base node through the resistor.
儘管第3圖之一替代方案可為將四個BJT電壓隨耦器裝置(345、365、360及375)改變成其對應極性的MOSFET,然而這樣可能導致DC位準相當容易改變,這是因為Vgs(on) 會隨主體電壓及額外雜訊(如1/f變化性)而改變。Although an alternative to FIG. 3 may be to change four BJT voltage follower devices (345, 365, 360, and 375) to their corresponding polarity MOSFETs, this may result in a DC level that is fairly easy to change because Vgs (on) will vary with the subject voltage and additional noise (such as 1/f variability).
因此,第3圖所示之電路需要一改良版本,使得不論使用何種特定電晶體組來實現電壓隨耦器,皆不會增加電壓隨耦器之偏壓電流位準。Therefore, the circuit shown in Figure 3 requires a modified version that does not increase the bias current level of the voltage follower regardless of the particular transistor set used to implement the voltage follower.
本發明之一態樣提供一種用於一CMOS時脈驅動器的設備,包含:一第一輸入接收電路,用於接收小訊號邏輯輸入;一第一電壓隨耦器電路,其係耦接至該第一輸入接收電路,以用於產生一第一組電壓隨耦器輸出;及一第一輸出電路,其係耦接至該第一電壓隨耦器電路,以用於接收該第一組電壓隨耦器輸出作為輸入,並產生輸出訊號,其中該第一電壓隨耦器電路係耦接至一第一切換電路,及該第一切換電路係連接至該第一組電壓隨耦器輸出,且係配置用於降低該等輸出訊號之相位雜訊位準。An aspect of the present invention provides an apparatus for a CMOS clock driver, comprising: a first input receiving circuit for receiving a small signal logic input; and a first voltage follower circuit coupled to the a first input receiving circuit for generating a first set of voltage follower outputs; and a first output circuit coupled to the first voltage follower circuit for receiving the first set of voltages The output of the follower is input, and an output signal is generated, wherein the first voltage follower circuit is coupled to a first switching circuit, and the first switching circuit is coupled to the first set of voltage follower outputs. And configured to reduce the phase noise level of the output signals.
本發明之另一態樣提供一種用於一時脈驅動器的設備,包含:一輸入接收電路,用於接收小訊號邏輯輸入;一電壓隨耦器電路,其係耦接至該輸入接收電路,以用於產生複數個電壓隨耦器輸出;及一輸出電路,其係耦接至該電壓隨耦器電路,以用於接收該複數個電壓隨耦器輸出作為輸入,並產生輸出訊號,其中該電壓隨耦器電路係耦接至一切換電路,及該切換電路係連接至該複數個電壓隨耦器輸出,且係配置用於降低該等輸出訊號之相位雜訊位準。Another aspect of the present invention provides an apparatus for a clock driver, comprising: an input receiving circuit for receiving a small signal logic input; and a voltage follower circuit coupled to the input receiving circuit to For generating a plurality of voltage follower outputs; and an output circuit coupled to the voltage follower circuit for receiving the plurality of voltage follower outputs as an input and generating an output signal, wherein the output signal is generated The voltage follower circuit is coupled to a switching circuit, and the switching circuit is coupled to the plurality of voltage follower outputs and configured to reduce phase noise levels of the output signals.
本發明一般而言係關於時脈驅動器電路。更特定言之,本發明係關於可改善時脈驅動器之相位雜訊表現的BiCMOS時脈驅動器電路。The present invention is generally directed to a clock driver circuit. More specifically, the present invention relates to a BiCMOS clock driver circuit that improves the phase noise performance of a clock driver.
本發明揭示一種適合用作時脈驅動器之電路,相較於前述先前技術電路之每一者,其具有降低的相位雜訊。藉由主動地往上或往下驅動第一MOSFET閘,在雙數子(ECL)部分與CMOS部分間之介面處達成改良。在某些具體實施例中,由一BJT射極隨耦器驅動一方向,而藉由使用一MOSFET切換器推動儲存於虛擬MOSFET閘之電荷來驅動另一方向。可瞭解到,依據本案申請專利範圍所載之範疇內的其它具體實施例亦是可能的。The present invention discloses a circuit suitable for use as a clock driver having reduced phase noise compared to each of the prior art circuits described above. An improvement is achieved at the interface between the double-numbered sub- (ECL) portion and the CMOS portion by actively driving the first MOSFET gate up or down. In some embodiments, a direction is driven by a BJT emitter follower, and the other direction is driven by using a MOSFET switch to push the charge stored in the dummy MOSFET gate. It will be appreciated that other specific embodiments within the scope of the scope of the patent application are also possible.
第4圖顯示一全差動與互補式電路400的示例性具體實施例,其由習知ECL邏輯閘來驅動一組MOSFET閘極端。與第3圖所示之電路300相比,電路400包括有額外的MOSFET於四個射極隨耦器427、430、440及443中每一者之輸出處。框470中包含新加入的MOSFET,即電晶體N5、N6、P3及P4(其為一組連接至射極隨耦器427及430之電晶體)及P5、P6、N3及N4(連接至射極隨耦器440及443)。FIG. 4 shows an exemplary embodiment of a fully differential and complementary circuit 400 that drives a set of MOSFET gate terminals by a conventional ECL logic gate. Circuit 400 includes an additional MOSFET at the output of each of the four emitter followers 427, 430, 440, and 443 as compared to circuit 300 shown in FIG. Block 470 includes newly added MOSFETs, namely transistors N5, N6, P3, and P4 (which are a set of transistors connected to emitter followers 427 and 430) and P5, P6, N3, and N4 (connected to the shot). Polar followers 440 and 443).
新加入的電晶體建構如下。電晶體N5係一NMOS裝置,其源極連接至一電流源I2,而其汲極連接至電晶體427(Q5)之射極。電晶體N6係一NMOS裝置,其源極連接至電流源I3,而其汲極連接至電晶體430(Q6)之射極。電晶體N5之閘極連接至電晶體N6之汲極,電晶體N6之閘極連接至電晶體N5之汲極。此為本發明之一重要特徵。如所揭示的,使用此一配置,電晶體N5及N6被建構作為切換器或所謂的切換器MOSFET。The newly added transistor is constructed as follows. The transistor N5 is an NMOS device having a source connected to a current source I2 and a drain connected to the emitter of the transistor 427 (Q5). The transistor N6 is an NMOS device having a source connected to the current source I3 and a drain connected to the emitter of the transistor 430 (Q6). The gate of transistor N5 is connected to the drain of transistor N6, and the gate of transistor N6 is connected to the drain of transistor N5. This is an important feature of the invention. As disclosed, with this configuration, transistors N5 and N6 are constructed as switches or so-called switch MOSFETs.
本發明另一重要特徵係關於置放在電晶體N5及N6之每一者的源極處的電容。如第4圖所示,一標示為P3的裝置係一PMOS電晶體,其汲極及源極連接至正供電軌,其閘極連接至電晶體N5之源極。同樣地,對於電晶體N6,一標示為P4的裝置係一PMOS電晶體,其汲極及源極連接至正供電軌,其閘極連接至電晶體N6之源極。裝置P3及P4之所欲功能為其每一者當作一電容,即一電荷儲存器。第4圖所示之連接使虛擬裝置P3及P4如電容般運作。Another important feature of the present invention relates to the capacitance placed at the source of each of transistors N5 and N6. As shown in FIG. 4, a device designated P3 is a PMOS transistor having a drain and a source connected to the positive supply rail and a gate connected to the source of the transistor N5. Similarly, for transistor N6, a device designated P4 is a PMOS transistor having its drain and source connected to the positive supply rail and its gate connected to the source of transistor N6. The desired function of devices P3 and P4 acts as a capacitor for each of them, i.e., a charge reservoir. The connection shown in Figure 4 causes virtual devices P3 and P4 to operate as capacitors.
至於第4圖所示電路的互補部分,電晶體P5係一PMOS裝置,其源極連接至一電流源I4而汲極連接至電晶體440(Q7)之射極。電晶體P6係一PMOS裝置,其源極連接至一電流源I5而汲極連接至電晶體443(Q8)之射極。同樣地,電晶體P5之閘極連接至電晶體P6之汲極,電晶體P6之閘極連接至電晶體P5之汲極。在此示例性實施例中,存在四個切換器MOSFET,分別標示為N5、N6、P5及P6。電晶體P5及P6結合當作切換器MOSFET,下文將進一步說明。對於電路400之互補部分也一樣,針對切換電路470中之電晶體P5及P6每一者,有一電容被配置於切換器MOSFET之每一者之源極處。如第4圖所示,裝置N3係一NMOS電晶體,其汲極及源極連接至負供電軌,而閘極連接至電晶體P5之源極。裝置N4係一NMOS電晶體,其汲極及源極連接至負供電軌,其閘極連接至電晶體P6之源極。電晶體N3及N4之每一者之角色為當作一電容,即電荷儲存器。使用第4圖所示之電路配置,N3及N4可達成如此的所欲功能。As for the complementary portion of the circuit shown in Fig. 4, the transistor P5 is a PMOS device having a source connected to a current source I4 and a drain connected to the emitter of the transistor 440 (Q7). The transistor P6 is a PMOS device having a source connected to a current source I5 and a drain connected to the emitter of the transistor 443 (Q8). Similarly, the gate of transistor P5 is connected to the drain of transistor P6, and the gate of transistor P6 is connected to the drain of transistor P5. In this exemplary embodiment, there are four switcher MOSFETs labeled N5, N6, P5, and P6, respectively. The transistors P5 and P6 are combined to act as a switch MOSFET, as will be further explained below. The same applies to the complementary portions of circuit 400. For each of transistors P5 and P6 in switching circuit 470, a capacitor is disposed at the source of each of the switch MOSFETs. As shown in FIG. 4, the device N3 is an NMOS transistor whose drain and source are connected to the negative supply rail and the gate is connected to the source of the transistor P5. The device N4 is an NMOS transistor having a drain and a source connected to the negative supply rail and a gate connected to the source of the transistor P6. Each of the transistors N3 and N4 functions as a capacitor, that is, a charge reservoir. Using the circuit configuration shown in Figure 4, N3 and N4 can achieve such a desired function.
如第4圖所示,電路400可適合操作成一邏輯轉譯器;然而,由於輸入端靜態且相等的電壓在輸出電晶體對(電晶體對445/455(N1/P1)及電晶體對450/460(N2/P2))中產生一射穿(shoot through),因此在某些實施例中,在第4圖所示的輸入之前可配置鎖存器或遲滯級(未圖示),以確保此等輸入不是處在ECL邏輯位準就是在邏輯位準間轉換。As shown in Figure 4, circuit 400 can be adapted to operate as a logic translator; however, since the input is static and equal in voltage at the output transistor pair (transistor pair 445/455 (N1/P1) and transistor pair 450/ A shoot through is generated in 460 (N2/P2), so in some embodiments, a latch or hysteresis stage (not shown) can be configured prior to the input shown in Figure 4 to ensure These inputs are either at the ECL logic level or at the logic level.
在電晶體402及410(Q1及Q3)之基極的輸入電壓高於電晶體405及412(Q2及Q4)之基極的輸入電壓的靜態中時,來自電流源415(I1)之電流被引導流經電晶體410(Q1)而到達電阻420(R3)。來自電流源407(I0)之電流被引導流經電晶體405(Q4)而到達電阻437(R2)。由於沒有電流流經電阻425(R4),PMOS P2之閘極電壓被NPN射極隨耦器430(Q6)朝正供電軌上拉,NMOS電晶體N5之閘極電壓亦同樣被上拉。來自電流源I2之電流因此流經電晶體N5,將PMOS電晶體445(P1)之閘極電壓下拉,直到NPN射極隨耦器427(Q5)導通為止。由於電流流經電阻420(R3),Q5將不導通,直到電晶體445(P1)之閘至源極電壓基本上大於一臨限Vgs為止,且因此完全增進裝置P1之效能。When the input voltage of the bases of transistors 402 and 410 (Q1 and Q3) is higher than the static input voltage of the bases of transistors 405 and 412 (Q2 and Q4), the current from current source 415 (I1) is The flow is directed through transistor 410 (Q1) to resistor 420 (R3). Current from current source 407 (I0) is directed through transistor 405 (Q4) to resistor 437 (R2). Since no current flows through resistor 425 (R4), the gate voltage of PMOS P2 is pulled up by the NPN emitter follower 430 (Q6) toward the positive supply rail, and the gate voltage of the NMOS transistor N5 is also pulled up. The current from current source I2 thus flows through transistor N5, pulling the gate voltage of PMOS transistor 445 (P1) down until the NPN emitter follower 427 (Q5) is turned on. Since current flows through resistor 420 (R3), Q5 will not conduct until the gate-to-source voltage of transistor 445 (P1) is substantially greater than a threshold Vgs, and thus the performance of device P1 is fully enhanced.
當電路仍處於處此靜態時,電晶體N6的閘極電壓係低於正供電軌一電壓值,該電壓值為I*R(電阻420(R3)之值)加上電晶體427(Q5)之Vbe值。維持此一狀態長達一段適當時間,電流源I3將P4(一電容連接裝置)的閘極電壓下拉至夠低,使得電晶體N6接著重新承載來自電流源I3之電流。然而,此並非對電路之操作要求,下文將進一步說明。When the circuit is still static, the gate voltage of the transistor N6 is lower than the voltage value of the positive supply rail, and the voltage value is I*R (the value of the resistor 420 (R3)) plus the transistor 427 (Q5). The Vbe value. Maintaining this state for an appropriate period of time, current source I3 pulls the gate voltage of P4 (a capacitive connection device) low enough that transistor N6 then reloads the current from current source I3. However, this is not an operational requirement for the circuit and will be further explained below.
在電路400下半部的相應電路中,當沒有任何電流流經電阻435(R1)時,NMOS電晶體455(N1)的閘極電壓被PNP射極隨耦器電晶體440(Q7)朝負供電軌下拉,PMOS電晶體P6之閘極電壓亦被下拉。來自電流源I5之電流因此被推動流經電晶體P6,將NMOS電晶體460(N2)之閘極電壓上拉,直到PNP射極隨耦器443(Q8)導通為止。由於電流流經電阻437(R2),Q8將不導通,直到電晶體460(N2)之閘至源極電壓基本上大於一臨限Vgs為止,且因此完全增進裝置N2之效能。In the corresponding circuit of the lower half of the circuit 400, when no current flows through the resistor 435 (R1), the gate voltage of the NMOS transistor 455 (N1) is negatively biased by the PNP emitter follower transistor 440 (Q7). When the power rail is pulled down, the gate voltage of the PMOS transistor P6 is also pulled down. The current from current source I5 is thus pushed through transistor P6, pulling up the gate voltage of NMOS transistor 460 (N2) until PNP emitter is turned on with 442 (Q8). Since current flows through resistor 437 (R2), Q8 will not conduct until the gate-to-source voltage of transistor 460 (N2) is substantially greater than a threshold Vgs, and thus the performance of device N2 is fully enhanced.
當電路仍處於處此靜態時,電晶體P5的閘極電壓係高於負供電軌組一電壓降,該電壓降測得為I*R(電阻437(R2)之值)加上電晶體443(Q8)之Vbe值。維持此一狀態長達一段適當時間,電流源I4將電晶體N3(一電容連接裝置)的閘極電壓上拉至夠高,使得電晶體P5重新承載來自電流源I4之電流。同樣地,此並非對電路之操作要求,下文將進一步說明。When the circuit is still in this static state, the gate voltage of the transistor P5 is higher than the voltage drop of the negative supply rail group, and the voltage drop is measured as I*R (the value of the resistor 437 (R2)) plus the transistor 443. The Vbe value of (Q8). Maintaining this state for a suitable period of time, current source I4 pulls up the gate voltage of transistor N3 (a capacitive connection device) high enough that transistor P5 re-bears the current from current source I4. Again, this is not an operational requirement for the circuit, as explained further below.
電路400所達成的改良最佳地表現在邏輯狀態間之轉換。由於電路400係全差動式,以上有關在一靜態邏輯時所發生的種種的描述,對相反的靜態邏輯而言皆為顛倒。同樣地,以下描述的功能係針對從上述之狀態轉換至一相反狀態的情況。對一相反狀況進行描述,反應了與轉換至上述靜態相關聯的情形。The improvements achieved by circuit 400 are best represented by the transition between logic states. Since circuit 400 is fully differential, the various descriptions described above with respect to a static logic are reversed for the opposite static logic. Likewise, the functions described below are directed to the transition from the above state to an opposite state. Describe the opposite situation and reflect the situation associated with transitioning to the above static.
在一轉換時,當連接至電晶體410(Q1)及402(Q3)之基極的輸入電壓下降低於電晶體412(Q2)及405(Q4)之基極的輸入電壓時,電流源407(I0)及415(I1)之電流被導引至相應差動對之集極上的另一相對電阻。對四個BJT射極隨耦器(電晶體427、430、440及443)之基極輸入端起反應的電路功能,係與參照第3圖所示電路300描述的功能相同。At a transition, when the input voltage to the bases of transistors 410 (Q1) and 402 (Q3) drops below the input voltage of the bases of transistors 412 (Q2) and 405 (Q4), current source 407 The currents of (I0) and 415 (I1) are directed to another relative resistance on the collector of the respective differential pair. The circuit function that reacts to the base inputs of the four BJT emitter followers (transistors 427, 430, 440, and 443) is the same as that described with reference to circuit 300 shown in FIG.
由於電晶體410(Q1)集極處之電流跌降,電阻420(R3)將電晶體427(Q5)之基極電壓上拉至正供電軌。由於電晶體427(Q5)係一射極隨耦器電晶體,因此其直接上拉電晶體445(P1)之閘極端,快速地將其關閉,如參照第3圖所述之情形。然而,電晶體427(Q5)亦上拉電路400中電晶體N6之閘極電壓。因為電晶體P4(電容連接裝置)被充電至比臨限Vgs大得多的一電壓,電晶體N6被開啟,其操作為一切換器將PMOS裝置P4及P2之閘極連接起來,以主動下拉輸出裝置450(P2)之閘極電壓。因為由輸入訊號(經由電晶體Q1-R3-Q5-N6)來主動地驅動,時間基雜訊與電流源I3之雜訊無關。Due to the current drop at the collector of transistor 410 (Q1), resistor 420 (R3) pulls the base voltage of transistor 427 (Q5) up to the positive supply rail. Since transistor 427 (Q5) is an emitter follower transistor, it directly pulls up the gate terminal of transistor 445 (P1) and quickly turns it off, as described with reference to Figure 3. However, transistor 427 (Q5) also pulls the gate voltage of transistor N6 in circuit 400. Since the transistor P4 (capacitor connection device) is charged to a voltage much larger than the threshold Vgs, the transistor N6 is turned on, and operates as a switch to connect the gates of the PMOS devices P4 and P2 to actively pull down The gate voltage of the output device 450 (P2). Since the input signal (via the transistors Q1-R3-Q5-N6) is actively driven, the time-based noise is independent of the noise of the current source I3.
在差動電路400之相應部分電路中,來自電流源415(I1)之電流被電晶體412(Q2)拉動並流經電阻425(R4),因此下拉射極隨耦器電晶體430(Q6)之基極電壓。如上述參照第3圖之說明,這樣無法確保電晶體450(P2)之閘極電壓被主動地拉低。然而,在電路400中,因為此處所述的N6切換器的操作,電晶體450(P2)之閘極電壓被快速拉低。由於電晶體450之閘極係處於一低電壓,電晶體N5被關閉,這是因為電容連接P3裝置使電晶體N5之源極端不會立即被電流源I2下拉。當電晶體P3之閘極被下拉至夠低時,電晶體N5接著開始傳導電流。發生此情況的確切時間點會因來自電流源I2的雜訊而變動(時間相關雜訊)。然而,這種來自電流源I2的雜訊不會影響輸出,因此訊號路徑之相位雜訊表現不會因電流源之雜訊而降級。In a corresponding portion of the circuit of the differential circuit 400, current from the current source 415 (I1) is pulled by the transistor 412 (Q2) and flows through the resistor 425 (R4), thus pulling down the emitter follower transistor 430 (Q6) Base voltage. As described above with reference to Fig. 3, it is not possible to ensure that the gate voltage of the transistor 450 (P2) is actively pulled low. However, in circuit 400, the gate voltage of transistor 450 (P2) is pulled low quickly due to the operation of the N6 switch described herein. Since the gate of the transistor 450 is at a low voltage, the transistor N5 is turned off because the capacitor is connected to the P3 device so that the source terminal of the transistor N5 is not immediately pulled down by the current source I2. When the gate of transistor P3 is pulled down sufficiently low, transistor N5 then begins to conduct current. The exact time at which this occurs will vary due to noise from current source I2 (time-related noise). However, this noise from current source I2 does not affect the output, so the phase noise performance of the signal path is not degraded by the noise of the current source.
此外,對電路400之下半部分而言,由於來自電晶體405(Q4)之集極的電流跌降,導致電晶體437(R2)將電晶體443(Q8)之基極電壓下拉至負供電軌。電晶體443(Q8)亦為一射極隨耦器,其接著直接下拉電晶體460(N2)之閘極電壓。如此可快速關閉電晶體460,如此處參照第3圖所述之情況。然而,在電路400中,電晶體443(Q8)亦下拉P5之閘極電壓。因為相較於P5之閘極電壓,電容連接裝置N3被充電至比臨限Vgs高出許多的一電壓,電晶體P5被開啟,其操作為一切換器將NMOS裝置N3及N1之閘極端連接起來。依此方式,電路400主動上拉輸出裝置N1之閘極電壓。此外,因為N1之閘極係由輸入訊號(經由Q4-R2-Q8-P5)主動驅動,時間基雜訊與電流源I4之雜訊無關。Moreover, for the lower half of circuit 400, transistor 437 (R2) pulls the base voltage of transistor 443 (Q8) to a negative supply due to the current drop from the collector of transistor 405 (Q4). rail. The transistor 443 (Q8) is also an emitter follower, which in turn directly pulls down the gate voltage of the transistor 460 (N2). This allows the transistor 460 to be quickly turned off, as described herein with reference to Figure 3. However, in circuit 400, transistor 443 (Q8) also pulls down the gate voltage of P5. Because the capacitor connection device N3 is charged to a voltage much higher than the threshold Vgs compared to the gate voltage of P5, the transistor P5 is turned on, and operates as a switch to connect the gate terminals of the NMOS devices N3 and N1. stand up. In this manner, circuit 400 actively pulls up the gate voltage of output device N1. In addition, since the gate of N1 is actively driven by the input signal (via Q4-R2-Q8-P5), the time-based noise is independent of the noise of current source I4.
至於電路400下半部之其它部分的操作,電流源407(I0)之電流被電晶體402(Q3)重新導向並流經電阻435(R1),因此上拉射極隨耦電晶體440(Q7)之基極電壓。如針對第3圖所示電路300之說明,這樣不能確保電晶體455(N1)之閘極電壓被主動地拉高。然而,在電路400中,由於此處所述的電晶體P5的相關切換器操作,電晶體455(N1)之閘極電壓被快速拉高。由於電晶體455之閘極電壓處於一較高電壓,電晶體P6被關閉,這是因為電容連接裝置N4使電晶體P6之源極端不會立即被電流源I5上拉。依此方式,僅當電晶體N4之閘極被拉得夠高時,電晶體P6重新傳導電流。發生此情況的確切時間點會因來自電流源I5的雜訊而變動。然而,此種雜訊不會影響輸出,因此訊號路徑之相位雜訊表現不會因電流源之雜訊而降級。As for the operation of the other portions of the lower half of the circuit 400, the current of the current source 407 (I0) is redirected by the transistor 402 (Q3) and flows through the resistor 435 (R1), so the pull-up emitter follows the coupling transistor 440 (Q7). The base voltage of ). As explained for the circuit 300 shown in FIG. 3, this does not ensure that the gate voltage of the transistor 455 (N1) is actively pulled high. However, in circuit 400, the gate voltage of transistor 455 (N1) is rapidly pulled high due to the associated switch operation of transistor P5 described herein. Since the gate voltage of the transistor 455 is at a higher voltage, the transistor P6 is turned off because the capacitor connection device N4 causes the source terminal of the transistor P6 to not be immediately pulled up by the current source I5. In this manner, transistor P6 re-conducts current only when the gate of transistor N4 is pulled high enough. The exact point in time at which this occurs will vary due to noise from current source I5. However, such noise does not affect the output, so the phase noise performance of the signal path is not degraded by the noise of the current source.
如此處所揭示之電路400之操作,所述之轉換具有被主動拉高的輸出裝置455(N1)及445(P1)二者的閘極電壓,及被被主動拉低的N1及P1之共用連接汲極,其皆具有最小的新增相位雜訊。此外,輸出裝置460(N2)及450(P2)二者之閘極電壓皆被主動拉低,且其共用連接汲極被主動地拉高,同時具有最小的新增相位雜訊。As with the operation of circuit 400 disclosed herein, the conversion has a gate voltage of both output devices 455 (N1) and 445 (P1) that are actively pulled high, and a common connection between N1 and P1 that are actively pulled low. Bungee, which has the smallest added phase noise. In addition, the gate voltages of both output devices 460 (N2) and 450 (P2) are actively pulled low, and their shared connection drains are actively pulled high with minimal added phase noise.
在本發明某些實施例中,所用的電容係實現成電容連接MOSFET,如第4圖所示,可選擇MOSFET的極性類型以匹配由電容主動連接的裝置的類型。例如,裝置P3係一PMOS裝置,其可被選擇來匹配PMOS裝置P1。同樣地,裝置P4係一PMOS類型,其匹配PMOS裝置P2。如此可更容易地以尺寸設計來控制此二者間的電容比例,同時亦可較有效地追蹤由於溫度及晶圓處理所導致的變異。然而,其它配置亦係可能的。舉例而言,所用的電容亦可使用不同建構方式來製成,諸如一平行板電容或一具有相反極性的二極體連接MOSFET。In some embodiments of the invention, the capacitors used are implemented as capacitor-connected MOSFETs, as shown in Figure 4, the polarity of the MOSFET can be selected to match the type of device actively connected by the capacitor. For example, device P3 is a PMOS device that can be selected to match PMOS device P1. Similarly, device P4 is a PMOS type that matches PMOS device P2. This makes it easier to size the capacitance ratio between the two, while also tracking the variation due to temperature and wafer processing more effectively. However, other configurations are also possible. For example, the capacitors used can also be fabricated using different construction methods, such as a parallel plate capacitor or a diode-connected MOSFET with opposite polarity.
在本發明之某些實施例中,為了多種原因可選擇其電容值大於輸出裝置電容值的電容連接MOSFET。例如,一輸出裝置之閘至汲極電容值會因米勒效應而倍增,而電容連接裝置不會經歷如此的米勒效應。在另一例中,輸出MOSFET及電容連接MOSFET二者之閘極每一者可在一整個訊號週期期間以相同電壓變化擺動。因此,在該二者之電容值被製成相等的情況下,當該二電容之間的MOSFET切換器關閉時造成電荷重分配而導致該二電容值經歷電壓變化,該電壓變化係該擺動的一半。由於輸出裝置之臨限Vgs一般係類似的但並非確切在一中途點(half-way point)處,因此希望能驅動輸出裝置閘極端超過電荷重分配之範圍內的中途點。此可由一大型電容連接裝置實現。In some embodiments of the invention, a capacitively connected MOSFET whose capacitance value is greater than the capacitance of the output device can be selected for a variety of reasons. For example, the gate-to-dip capacitance value of an output device is multiplied by the Miller effect, and the capacitive connection device does not experience such a Miller effect. In another example, the gates of both the output MOSFET and the capacitor-connected MOSFET can each swing with the same voltage change during the entire signal period. Therefore, in the case where the capacitance values of the two are made equal, when the MOSFET switch between the two capacitors is turned off, the charge redistribution is caused to cause the two capacitance values to undergo a voltage change, and the voltage change is the swing. half. Since the threshold Vgs of the output device is generally similar but not exactly at a half-way point, it is desirable to be able to drive the output device gate terminal beyond the midway point within the range of charge redistribution. This can be achieved by a large capacitive connection device.
一較大電容連接裝置可能存在一些相關問題。例如,發生在一非主動(inactive)轉換後的重新充電通常需要較長時間。相同充電時間所需的靜態電流可能增加。例如,若一電容連接裝置之電容值並未比輸出裝置之電容值大50%以上或大100%,則相較於第3圖所示電路為了得到相同轉換速度且仍保有改善相雜訊所需的電流,所汲取的額外電流係小的。A large capacitive connection device may have some related problems. For example, recharging after an inactive transition typically takes a long time. The quiescent current required for the same charging time may increase. For example, if the capacitance value of a capacitor connection device is not more than 50% larger or larger than the capacitance value of the output device, the circuit shown in FIG. 3 maintains the same conversion speed and still maintains an improved phase noise. The current required, the extra current drawn is small.
電路400的另一相關特徵說明如下。電阻上的電壓擺動,加上射極隨耦器的Vbe值,再加上切換器MOSFET的Vgs值,所得值接近一等於或超過總供應電壓的電壓值。例如,當電路400可操作在一5V電壓供應上時,其亦適合以一3.3V供應電壓操作。在工業標準10%的容差下,所供應的電壓可低達3V。在電阻處具有800mVp-p擺動及射極隨耦器具有800mV的Vbe情況下,可消耗超過一半的供應電壓。Another related feature of circuit 400 is illustrated below. The voltage swing across the resistor, plus the Vbe value of the emitter follower, plus the Vgs value of the switch MOSFET, is close to a voltage value equal to or exceeding the total supply voltage. For example, when circuit 400 is operable to operate on a 5V supply, it is also suitable for operation with a 3.3V supply voltage. Under the industry standard 10% tolerance, the supplied voltage can be as low as 3V. With a 800mVp-p swing at the resistor and a Vbe with an emitter follower of 800mV, more than half of the supply voltage can be consumed.
切換器MOSFET可以源極遠離電軌(主體一般常聯結至該電軌)的方式操作。如此會增加臨限電壓Vgs,除非主體可浮接(float)並聯結至源極端。在某些實例中,這不是一定可行的,而在某些情況下,這可能是不想要發生的情形。在BJT Vbe為900mV及MOSFET Vgs可能為1.2V時所處溫度的最糟情況下,從電軌起算的總電壓橫跨2.9V,僅為電流源I2-I5留下100mV的餘裕(headroom)。在存在接地彈跳(bounce)或其它動態擺動的情況下,此寬限可能完全消逝。The switch MOSFET can operate in a manner that the source is remote from the rail (the body is typically coupled to the rail). This will increase the threshold voltage Vgs unless the body can float to the source terminal in parallel. In some instances, this is not necessarily possible, and in some cases this may be a situation that does not want to happen. In the worst case of the temperature at which the BJT Vbe is 900mV and the MOSFET Vgs may be 1.2V, the total voltage from the rail straddles 2.9V, leaving only 100mV of headroom for the current source I2-I5. In the presence of a ground bounce or other dynamic wobble, this grace may completely disappear.
上述問題即使存在,就電路400而言並非致命的,原因如下。一電流源當符合餘裕(compliance headroom)不足時會良性跌降(例如,以MOSFET輸出裝置實現的電流源),在電路400中一般可接受這種電流源。雖然電容連接MOSFET可停止充電,然而在停止充電那一刻,此一電容連接MOSFET可能已具有大部分的所需電壓變化,因此已儲存了大部分所需電荷。在此情況下,不需要使切換器MOSFET導通電流。這可消除射極隨耦器在其汲極上之偏壓,這是由於在轉換時射極隨耦器對輸出MOSFET之Cgs放電,且可具有足夠的偏壓電流量以將電荷拉出。The above problem, if any, is not fatal for circuit 400 for the following reasons. A current source can be a benign drop when it meets a deficiency in the compliance headroom (e.g., a current source implemented with a MOSFET output device) that is generally acceptable in circuit 400. Although the capacitor-connected MOSFET can stop charging, at the moment the charging is stopped, the capacitor-connected MOSFET may already have most of the required voltage change, so most of the required charge has been stored. In this case, there is no need to cause the switch MOSFET to conduct current. This eliminates the bias of the emitter follower on its drain because the emitter follower discharges the Cgs of the output MOSFET during switching and can have a sufficient amount of bias current to pull the charge out.
在轉換完成後,Q5-Q8的射極可只是保持閒置而不會有負面副作用。若在一節點處有漏電流,電壓可能漂移,導致異常行為或限制操作的最低頻率。若在一特定應用無法接受這情形,可加入一小型電流源以解決此問題。此一加入的電流源可設置成電流源I2-I5之值的十分之一或少於電流源I2-I5之值,以能夠獨立提供最小偏壓位準給每一射極隨耦器。因為相較於I2-I5的連接,Q5-Q8的射極係在切換器MOSFET的另一側,通常具有大量餘裕給此類小型額外電流源。After the conversion is complete, the emitter of the Q5-Q8 can simply remain idle without negative side effects. If there is leakage current at a node, the voltage may drift, causing abnormal behavior or limiting the minimum frequency of operation. If this is not acceptable in a particular application, a small current source can be added to solve the problem. The added current source can be set to one tenth of the value of the current source I2-I5 or less than the value of the current source I2-I5 to be able to independently provide a minimum bias level to each emitter follower. Because the emitter of Q5-Q8 is on the other side of the switch MOSFET compared to the I2-I5 connection, it typically has a large margin for such small additional current sources.
在第4圖所示的示例性實施例中,電容連接MOSFET係連接至用於個別半電路中的供應電壓。應瞭解到,此配置並非必要,本發明可實現為將此類電容連接至任何靜態或準靜態節點。如本領域所熟知的,CMOS電路系統在轉換期間從電壓供應軌引起大的電流尖波,因此可在電源供應上造成相當大的電壓「彈跳」。電路系統400之示例配置某種程度上對此情況免疫。In the exemplary embodiment shown in FIG. 4, the capacitive connection MOSFET is connected to a supply voltage for use in an individual half circuit. It should be appreciated that this configuration is not necessary and the present invention can be implemented to connect such capacitors to any static or quasi-static node. As is well known in the art, CMOS circuitry causes large current spikes from the voltage supply rail during the transition, thus causing a substantial voltage "bounce" on the power supply. An example configuration of circuitry 400 is somewhat immune to this situation.
納入切換器MOSFET N5、N6、P5及P6,可因此藉由全力加速MOSFET N1、N2、P1及P2之開啟速度,來改善電路400之效能,使其比電路300之效能更佳。一般而言,他們不負責關閉MOSFET N1、N2、P1及P2,而電路400中的射極隨耦器Q5、Q6、Q7及Q8使其關閉快速。切換器MOSFET會在關鍵轉換(即,其中一特定切換器MOSFET正開啟其相關聯的MOSFET N1、N2、P1或P2的轉換)中適當時間造成來自相應電容連接MOSFET的電流激增。切換器MOSFET在其它轉換期間並非關鍵。切換器MOSFET N5及P6在開啟裝置P1及N2的轉換期間係關鍵的。切換器MOSFET N6及P5在開啟裝置P2及N1的轉換期間係關鍵的。Incorporating the switch MOSFETs N5, N6, P5, and P6, the efficiency of the circuit 400 can be improved by the full speed of the turn-on speeds of the MOSFETs N1, N2, P1, and P2, making it more efficient than the circuit 300. In general, they are not responsible for turning off MOSFETs N1, N2, P1, and P2, while the emitters in circuit 400 follow the couplers Q5, Q6, Q7, and Q8 to turn them off quickly. The switch MOSFETs cause a surge in current from the corresponding capacitor-connected MOSFET at the appropriate time in a critical transition (ie, where a particular switch MOSFET is turning on its associated MOSFET N1, N2, P1, or P2 transition). The switch MOSFET is not critical during other conversions. Switcher MOSFETs N5 and P6 are critical during the switching of turn-on devices P1 and N2. Switcher MOSFETs N6 and P5 are critical during the switching of turn-on devices P2 and N1.
需注意到,切換器MOSFET電晶體N5、N6、P5及P6的設計標準可與電路400中所示的其它MOSFET大大不同。每一切換器MOSFET在關鍵轉換時被驅動作為一切換器,並在其它轉換時關閉,僅在其間的閒置時間期間具有主動線性操作。在這些情況中,任何位置的此一切換器MOSFET的雜訊並非與輸出MOSFET或BJT電晶體的雜訊幾乎一樣重要。因此,當輸出裝置(例如,P1、P2、N1及N2)需要設計成具有最小可能雜訊時,可基於諸如切換速度或通道電阻的其它標準來最佳化切換器MOSFET。It is noted that the design criteria for the switch MOSFET transistors N5, N6, P5, and P6 can be significantly different than the other MOSFETs shown in circuit 400. Each switch MOSFET is driven as a switch during critical transitions and is turned off during other transitions, with active linear operation only during idle time. In these cases, the noise of this switch MOSFET at any location is not as important as the noise of the output MOSFET or BJT transistor. Thus, when the output devices (eg, P1, P2, N1, and N2) need to be designed to have the least possible noise, the switch MOSFET can be optimized based on other criteria such as switching speed or channel resistance.
為了完全利用本發明之優點,第4圖所示之電路400可以可儘可能快速地轉換的輸入來驅動。如前所述,當因其它原因而可適用此特性時,具有鎖存器或遲滯作用的一前級可能足以確保轉換可快速發生。In order to fully utilize the advantages of the present invention, the circuit 400 shown in FIG. 4 can be driven with an input that can be converted as quickly as possible. As mentioned earlier, when this feature is applicable for other reasons, a pre-stage with a latch or hysteresis may be sufficient to ensure that the conversion can occur quickly.
相較於第3圖所示的習知電路300,第4圖所示的電路400在實體實現上亦係有利的。一般由用於高速電路設計的輸出電容所控制的第3圖中電流源I2-I5(350、367、352及370)之輸出阻抗,直接影響電路300之相位雜訊表現。這是因為第3圖中的此等電流源降低輸出閘驅動節點的偏斜率(skew rate)。然而,依據本發明,如第4圖所示的四個電流源I2-I5具有一電容與其連接,且該電容為此處所述之改良的一部分。採用此種電路配置,電流源之輸出電容就不那麼重要,而第4圖中電流源I2-I5的輸出電容可實際幫助改善相位雜訊表現。Compared to the conventional circuit 300 shown in FIG. 3, the circuit 400 shown in FIG. 4 is also advantageous in physical implementation. The output impedance of current source I2-I5 (350, 367, 352, and 370) in Figure 3, which is typically controlled by the output capacitor for high speed circuit design, directly affects the phase noise performance of circuit 300. This is because these current sources in Figure 3 reduce the skew rate of the output gate drive node. However, in accordance with the present invention, the four current sources I2-I5 as shown in Figure 4 have a capacitor connected thereto and which is part of the improvement described herein. With this circuit configuration, the output capacitance of the current source is less important, and the output capacitance of the current source I2-I5 in Figure 4 can actually help improve phase noise performance.
在第4圖所示的示例性實現中,類似電路元件之值一般可製成相同或相近。例如,R3=R4=R1=R2,I0=I1,且I2=I3=I4=I5。此外,為了差動對稱性,I2=I3,I4=I5,R3=R4,且R1=R2。然而,應瞭解到,在示例性實施例中不需要其它的一致性或相似性。例如,在NPN速度比PNP速度快得多的程序中,相對於下半部電路(435及437),針對上半部電路(420及425)偏斜電流源I2-I5及電阻之間的關係係有利的。進行此一偏斜的另一原因可為─存在NMOS對PMOS臨限Vgs的極度不平衡狀態,在此情況下所欲乘積I1×R3可相對於乘積I0×R1而偏斜。此設計變化全部係在本發明範疇內。可基於NMOS與PMOS雜訊表現的差異來建立對輸出MOSFET裝置通道長度及寬度的較佳偏斜。也就是說,NMOS及PMOS裝置N1、N2及P1、P2需要不同的幾何尺寸(長度、寬度),使得該二對裝置之雜訊位準係可比較的。In the exemplary implementation shown in FIG. 4, the values of similar circuit components can generally be made the same or similar. For example, R3 = R4 = R1 = R2, I0 = I1, and I2 = I3 = I4 = I5. Further, for differential symmetry, I2 = I3, I4 = I5, R3 = R4, and R1 = R2. However, it should be appreciated that no other consistency or similarity is required in the exemplary embodiments. For example, in a program where the NPN speed is much faster than the PNP speed, the relationship between the skew current source I2-I5 and the resistance for the upper half circuits (420 and 425) with respect to the lower half circuits (435 and 437). It is advantageous. Another reason for performing this skew may be that there is an extremely unbalanced state of the NMOS to PMOS threshold Vgs, in which case the desired product I1 × R3 may be skewed relative to the product I0 × R1. This design change is all within the scope of the invention. The preferred skew of the channel length and width of the output MOSFET device can be established based on the difference in NMOS and PMOS noise performance. That is, the NMOS and PMOS devices N1, N2, and P1, P2 require different geometries (length, width) such that the noise levels of the two pairs of devices are comparable.
第5圖顯示依本發明之一實施例的一全差動與互補式電路的實施範例,其用於由習知ECL邏輯驅動一組MOSFET閘極端以產生標準LVDS邏輯訊號。此電路產生具有第4圖的相位雜訊改良的低電壓差動訊號(Low Voltage Differential Signaling,LVDS)輸出。Figure 5 shows an embodiment of a fully differential and complementary circuit for driving a set of MOSFET gates by conventional ECL logic to generate standard LVDS logic signals in accordance with an embodiment of the present invention. This circuit produces a low voltage differential signaling (LVDS) output with phase noise improvement as shown in FIG.
LVDS係由TIA/EIA-644-A標準定義,且一般會需要比第5圖所示電路更多的電路,例如主動控制至少一3.5mA電流源以確保輸出偏移電壓(定義於標準中)符合規格4.1.2。用於執行此功能的電路系統及其它符合規定所必需的物,可屬於習知結構而仍能實現第5圖的相位雜訊改善。LVDS is defined by the TIA/EIA-644-A standard and generally requires more circuitry than the circuit shown in Figure 5, such as actively controlling at least a 3.5 mA current source to ensure output offset voltage (defined in the standard). Meet the specifications 4.1.2. The circuitry used to perform this function and other items necessary for compliance may be of conventional construction while still achieving phase noise improvement in FIG.
藉由引導3.5mA電流源通過N9及N12操控N通道MOSFET或通過N10及N11操控N通道MOSFET,來產生LVDS訊號。當在LVDS接收器處結合100歐姆差動終端時,可依此方式產生一為350mV的差動電壓。為了開啟NMOS裝置N9及N12,其閘極節點(其與P1及N7之汲極聯結)必需被拉高。為了開啟NMOS裝置N10及N11,其閘極節點(其與P2及N8之汲極聯結)必需被拉高。The LVDS signal is generated by directing a 3.5 mA current source to operate the N-channel MOSFET through N9 and N12 or by manipulating the N-channel MOSFET through N10 and N11. When a 100 ohm differential terminal is incorporated at the LVDS receiver, a differential voltage of 350 mV can be generated in this manner. In order to turn on the NMOS devices N9 and N12, their gate nodes (which are connected to the drains of P1 and N7) must be pulled high. In order to turn on the NMOS devices N10 and N11, their gate nodes (which are connected to the drains of P2 and N8) must be pulled high.
第5圖之操作與第4圖上四個標示為N1、N2、P1及P2的MOSFET之操作相同。第4圖中電路可用於驅動操控MOSFET N5-N8,以產生LVDS訊號。然而,在轉換期間,當只有裝置N11及N12開啟而N9及N10未開啟時,存在一短暫瞬時。當只有N11及N12開啟時,低3.5mA電流槽可以動態方式下拉輸出線,可能導致難以符合LVDS標準之規格4.1.5─動態輸出訊號平衡。The operation of Figure 5 is identical to the operation of the four MOSFETs labeled N1, N2, P1, and P2 on Figure 4. The circuit in Figure 4 can be used to drive the MOSFETs N5-N8 to generate LVDS signals. However, during the transition, there is a brief instant when only devices N11 and N12 are turned on and N9 and N10 are not turned on. When only N11 and N12 are turned on, the low 3.5mA current sink can dynamically pull down the output line, which may make it difficult to meet the LVDS standard specification 4.1.5 - Dynamic Output Signal Balance.
分別將N7及N8 NMOS裝置加入至N1及N2之汲極中,改變當產生LVDS訊號時的動態行為。明確地說,在P1之汲極由低位準升至高位準而因此P2的汲極由高位準降至低位準的轉換中,一旦電壓隨耦器Q5及切換器MOSFET N5拉低P1之閘極,則P1之汲極會上升。然而,與第4圖不同的是,一旦電壓隨耦器Q8及切換器MOSFET P6拉高N2之閘極,則P2之汲極會被拉低。此外,P1之汲極電壓必需升高以足以開啟交叉耦合裝置N8。此時,N2之汲極能夠拉低P2之汲極。The N7 and N8 NMOS devices are added to the drains of N1 and N2, respectively, to change the dynamic behavior when the LVDS signal is generated. Specifically, the pole of P1 rises from the low level to the high level, so the pole of P2 drops from the high level to the low level. Once the voltage follower Q5 and the switch MOSFET N5 pull the gate of P1 low. Then, the bungee of P1 will rise. However, unlike Figure 4, once the voltage follower Q8 and the switch MOSFET P6 pull up the gate of N2, the drain of P2 is pulled low. In addition, the drain voltage of P1 must be raised enough to turn on the cross-coupling device N8. At this point, the N2's bungee can pull down the P2's bungee.
藉由提供具有在下降邊緣(而非在上升邊緣)延遲的閘極驅動訊號的操控NMOS裝置N9-N12,動態輸出訊號平衡被改善。當P1之汲極的上升速度比P2之汲極的下降速度快時,N9及N10關閉的時間長度會大大縮短或基本上為零。The dynamic output signal balance is improved by providing a steering NMOS device N9-N12 having a gate drive signal that is delayed at the falling edge (rather than at the rising edge). When the rising speed of the pole of P1 is faster than the falling speed of the pole of P2, the length of time for N9 and N10 to be turned off is greatly shortened or substantially zero.
第6圖顯示依本發明之一實施例的一全差動與互補式電路的另一不同實施例,其用於由習知ECL邏輯驅動一組MOSFET閘極端以產生標準LVDS邏輯訊號。在電路600中,用於從N1、N2、P1及P2提供的CMOS驅動轉換至一LVDS輸出的輸出部分,係由第5圖所示的其之鏡像替代。Figure 6 shows a different embodiment of a fully differential and complementary circuit in accordance with an embodiment of the present invention for driving a set of MOSFET gate terminals by conventional ECL logic to generate standard LVDS logic signals. In circuit 600, the output portion for switching from the CMOS driver provided by N1, N2, P1, and P2 to an LVDS output is replaced by the image shown in FIG.
第6圖中之操控MOSFET現為PMOS裝置P9至P12,動態輸出訊號平衡可惡化到裝置P11及P12會關閉而裝置P9或P10會開啟的程度。第6圖採用與第5圖之電路500所達目的相同的功能方法來降低此惡化情形發生,其係藉由改變閘驅動訊號之邊緣之時間來達成。在此例中,如同N1及N2之汲極,交叉耦合裝置P7及P8延遲訊號之上升邊緣而非下降邊緣。The control MOSFET in Figure 6 is now PMOS devices P9 to P12, and the dynamic output signal balance can be degraded to the extent that devices P11 and P12 will be turned off and device P9 or P10 will be turned on. Figure 6 uses the same functional approach as the circuit 500 of Figure 5 to reduce this degradation by achieving a change in the edge of the gate drive signal. In this example, as with the drains of N1 and N2, the cross-coupling devices P7 and P8 delay the rising edge of the signal rather than the falling edge.
在某些情況下,第6圖所示的電路600可能會遭遇到一些問題。例如,在TIA/EIA-644-A標準下的低位準輸出可能比接地點還小1V,而不足以完全增進操控裝置P11及P12之效能。一般而言,可能需要浮接井(well)以避免主體效應(bulk effect)。然而,相較於驅動第5圖中之操控裝置N9及N10,一被供給1.8V電源供應的裝置可更輕易解決此問題。In some cases, circuit 600 shown in Figure 6 may encounter some problems. For example, a low level output under the TIA/EIA-644-A standard may be 1V less than the ground point, and is not sufficient to fully enhance the performance of the controls P11 and P12. In general, a well may be required to avoid a bulk effect. However, a device that is supplied with a 1.8V power supply can more easily solve this problem than the driving devices N9 and N10 in Fig. 5.
存在多種實現方式來實施本發明。例如,可將第4-6圖中包含P1及P2驅動電路的上半部電路與第2圖之輸出連接結合使用,以產生可提供與第1圖之電路相比具有改良的相位雜訊位準的一電路。雖然輸入差動電晶體對402、410、405及412(Q1及Q4)顯示為BJT,然而其亦可應用MOSFET來實現。為了節省電源,第4-6圖所示的I2-I5電流源可依據電路之操作頻率而動態地改變。或者,可使用一非線性電流源,一旦電容連接MOSFET被充分充電時,其可降至一較低閒置值。There are a variety of implementations to implement the invention. For example, the upper half of the P1 and P2 driver circuits in Figures 4-6 can be used in conjunction with the output connections of Figure 2 to provide improved phase noise bits compared to the circuit of Figure 1. A quasi-circuit. Although the input differential transistor pairs 402, 410, 405, and 412 (Q1 and Q4) are shown as BJTs, they can also be implemented using MOSFETs. To conserve power, the I2-I5 current source shown in Figures 4-6 can be dynamically changed depending on the operating frequency of the circuit. Alternatively, a non-linear current source can be used which can be reduced to a lower idle value once the capacitor-connected MOSFET is fully charged.
亦可將電壓隨耦器從BJT射極隨耦器改變成MOSFET或甚至JFET源極隨耦器。PNP/P-FET對NPN/N-FET的極性不變,且接至電路的電壓隨耦器連接亦不變。如本領域所熟知的,由於Vbe及Vgs(on) 位準不同,需要對偏壓位準進行某些小的改變。要進行此一替換,電壓隨耦器輸入端由一BJT基極改變成一FET閘極,輸出端由一BJT射極改變成一FET源極,而電源供應端由一BJT集極改變成一FET汲極。The voltage follower can also be changed from a BJT emitter follower to a MOSFET or even a JFET source follower. The polarity of the PNP/P-FET is unchanged for the NPN/N-FET, and the voltage connected to the circuit does not change with the coupler connection. As is well known in the art, some small changes to the bias level are required due to the different Vbe and Vgs (on) levels. To perform this replacement, the voltage follower input is changed from a BJT base to a FET gate, the output is changed from a BJT emitter to a FET source, and the power supply is changed from a BJT collector to a FET drain. .
所例示的實現方式具有相容於ECL(emitter-coupled logic,射極耦接邏輯)的輸入。近年來,CML(current-mode logci,電流模式邏輯)激增。本領域之技藝人士同意,可採用省略輸入處的差動對並將差動電流饋送給電阻R1至R4的替代方案。當然,藉由在必要時使用適當的位準轉換及阻抗改變,來調適輸入接收電路以接受任何小訊號邏輯輸入訊號,這種作法應為可能的。The illustrated implementation has an input that is compatible with ECL (emitter-coupled logic). In recent years, CML (current-mode logci) has proliferated. Those skilled in the art will appreciate that alternatives may be employed that omit the differential pair at the input and feed the differential current to resistors R1 through R4. Of course, it should be possible to adapt the input receiving circuit to accept any small signal logic input signal by using appropriate level conversion and impedance changes as necessary.
第4-6圖包括本領域技藝人士所熟知的電流源,其可使用BJT或MOSFET來實現,在某些例子中甚至可僅使用電阻來實現。Figures 4-6 include current sources well known to those skilled in the art, which may be implemented using BJT or MOSFETs, and in some instances may even be implemented using only resistors.
本發明已參照某些特定示例性實施例進行說明,其中之用語僅作為一般敘述性用語,不應視為限制性用語。在所附申請專利範圍之範疇內,可對本發明進行修改而不會悖離本發明各方面之範疇或精神。雖然已參照特定結構、動作及材料來描述本發明,不應將本發明限制於所揭示的特定特徵,而可以多種形式來實作,其中某些實作方式可能與此處所揭露之實施例相當不同,且本發明之範疇延伸至所有均等結果、動作及材料,如同包含於所附申請專利範圍之範疇內。The invention has been described with reference to certain specific exemplary embodiments, which are to be construed as a The invention may be modified within the scope of the appended claims without departing from the scope or spirit of the invention. Although the present invention has been described with reference to the specific structures, acts and materials, the present invention is not limited to the specific features disclosed, but may be practiced in various forms, some of which may be equivalent to the embodiments disclosed herein. The scope of the present invention extends to all equal results, actions, and materials as are included within the scope of the appended claims.
100...電路100. . . Circuit
105...電阻105. . . resistance
110...電阻110. . . resistance
115...電晶體115. . . Transistor
120...電晶體120. . . Transistor
125...偏壓電流125. . . Bias current
130...射極隨耦器130. . . Emitter follower
135...射極隨耦器135. . . Emitter follower
140...偏壓電流140. . . Bias current
145...偏壓電流145. . . Bias current
150...PMOS150. . . PMOS
155...PMOSFET155. . . PMOSFET
200...電路200. . . Circuit
210...PMOSFET210. . . PMOSFET
220...PMOSFET220. . . PMOSFET
230...CMOS反相器230. . . CMOS inverter
240...CMOS反相器240. . . CMOS inverter
300...電路300. . . Circuit
305...偏壓電流305. . . Bias current
310...輸入電晶體310. . . Input transistor
315...輸入電晶體315. . . Input transistor
320...輸入電晶體320. . . Input transistor
325...輸入電晶體325. . . Input transistor
330...偏壓電流330. . . Bias current
335...電阻335. . . resistance
340...電阻340. . . resistance
345...電壓隨耦器345. . . Voltage follower
350...電流源350. . . Battery
352...電流源352. . . Battery
355...電阻355. . . resistance
357...電阻357. . . resistance
360...電壓隨耦器360. . . Voltage follower
365...電壓隨耦器365. . . Voltage follower
367...電流源367. . . Battery
370...電流源370. . . Battery
375...電壓隨耦器375. . . Voltage follower
377...PMOSFET377. . . PMOSFET
380...PMOSFET380. . . PMOSFET
385...NMOSFET385. . . NMOSFET
390...NMOSFET390. . . NMOSFET
400...全差動與互補式電路400. . . Fully differential and complementary circuits
402...電晶體402. . . Transistor
405...電晶體405. . . Transistor
407...電流源407. . . Battery
410...電晶體410. . . Transistor
412...電晶體412. . . Transistor
415...電流源415. . . Battery
420...電阻420. . . resistance
425...電阻425. . . resistance
427...射極隨耦器427. . . Emitter follower
430...射極隨耦器430. . . Emitter follower
435...電阻435. . . resistance
437...電阻437. . . resistance
440...射極隨耦器440. . . Emitter follower
443...射極隨耦器443. . . Emitter follower
445...PMOSFET445. . . PMOSFET
450...PMOSFET450. . . PMOSFET
455...NMOSFET455. . . NMOSFET
460...NMOSFET460. . . NMOSFET
470...切換電路470. . . Switching circuit
500...電路500. . . Circuit
502...電晶體502. . . Transistor
505...電晶體505. . . Transistor
507...電流源507. . . Battery
510...電晶體510. . . Transistor
512...電晶體512. . . Transistor
515...電流源515. . . Battery
520...電阻520. . . resistance
525...電阻525. . . resistance
527...射極隨耦器527. . . Emitter follower
530...射極隨耦器530. . . Emitter follower
535...電阻535. . . resistance
537...電阻537. . . resistance
540...射極隨耦器540. . . Emitter follower
543...射極隨耦器543. . . Emitter follower
545...PMOSFET545. . . PMOSFET
550...PMOSFET550. . . PMOSFET
555...NMOSFET555. . . NMOSFET
560...NMOSFET560. . . NMOSFET
570...切換電路570. . . Switching circuit
600...電路600. . . Circuit
602...電晶體602. . . Transistor
605...電晶體605. . . Transistor
607...電流源607. . . Battery
610...電晶體610. . . Transistor
612...電晶體612. . . Transistor
615...電流源615. . . Battery
620...電阻620. . . resistance
625...電阻625. . . resistance
627...射極隨耦器627. . . Emitter follower
630...射極隨耦器630. . . Emitter follower
635...電阻635. . . resistance
637...電阻637. . . resistance
640...射極隨耦器640. . . Emitter follower
643...射極隨耦器643. . . Emitter follower
645...PMOSFET645. . . PMOSFET
650...PMOSFET650. . . PMOSFET
655...NMOSFET655. . . NMOSFET
660...NMOSFET660. . . NMOSFET
670...切換電路670. . . Switching circuit
此處主張及(或)描述之本發明已如前述以範例實施例進一步說明,並參照圖示詳細描述這些範例實施例,這些實施例並非限制性的範例實施例。在數個所有圖示中,類似元件符號代表類似結構。The present invention has been described and illustrated in the foregoing, by way of example, the exemplary embodiments, In all of the figures, like element symbols represent similar structures.
第1圖(先前技術)圖示用於由習知ECL邏輯驅動一PMOS閘對的一電路;Figure 1 (Prior Art) illustrates a circuit for driving a PMOS gate pair by conventional ECL logic;
第2圖(先前技術)顯示用以產生習知CMOS邏輯訊號之先前技術手段;Figure 2 (Prior Art) shows prior art means for generating conventional CMOS logic signals;
第3圖(先前技術)顯示一電路之全差動與互補實現,該電路用以由ECL邏輯驅動一組MOSFET閘極端以產生習知CMOS邏輯訊號;Figure 3 (Prior Art) shows a fully differential and complementary implementation of a circuit for driving a set of MOSFET gates by ECL logic to generate conventional CMOS logic signals;
第4圖顯示依據本發明之具體實施例之一全差動與互補式電路之示例性具體實施例,該電路用以由習知ECL邏輯驅動一組MOSFET閘極端以產生習知CMOS邏輯訊號;4 shows an exemplary embodiment of a fully differential and complementary circuit in accordance with an embodiment of the present invention for driving a set of MOSFET gate terminals by conventional ECL logic to generate conventional CMOS logic signals;
第5圖顯示依據本發明之具體實施例之一全差動與互補式電路之示例性具體實施例,該電路用以由習知ECL邏輯驅動一組MOSFET閘極端以產生標準LVDS邏輯訊號;及Figure 5 shows an exemplary embodiment of a fully differential and complementary circuit in accordance with an embodiment of the present invention for driving a set of MOSFET gates by conventional ECL logic to generate standard LVDS logic signals;
第6圖顯示依據本發明之具體實施例之一全差動與互補式電路之另一替代具體實施例,該電路用以由習知ECL邏輯驅動一組MOSFET閘極端以產生標準LVDS邏輯訊號。Figure 6 shows another alternative embodiment of a fully differential and complementary circuit in accordance with an embodiment of the present invention for driving a set of MOSFET gate terminals by conventional ECL logic to produce a standard LVDS logic signal.
400...全差動與互補式電路400. . . Fully differential and complementary circuits
402...電晶體402. . . Transistor
405...電晶體405. . . Transistor
407...電流源407. . . Battery
410...電晶體410. . . Transistor
412...電晶體412. . . Transistor
415...電流源415. . . Battery
420...電阻420. . . resistance
425...電阻425. . . resistance
427...射極隨耦器427. . . Emitter follower
430...射極隨耦器430. . . Emitter follower
435...電阻435. . . resistance
437...電阻437. . . resistance
440...射極隨耦器440. . . Emitter follower
443...射極隨耦器443. . . Emitter follower
445...PMOSFET445. . . PMOSFET
450...PMOSFET450. . . PMOSFET
455...NMOSFET455. . . NMOSFET
460...NMOSFET460. . . NMOSFET
470...切換電路470. . . Switching circuit
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US7646219B2 (en) * | 2008-06-05 | 2010-01-12 | Texas Instruments Incorporated | Translator circuit having internal positive feedback |
-
2009
- 2009-11-24 US US12/624,854 patent/US7969189B2/en active Active
-
2010
- 2010-11-24 EP EP10014953.3A patent/EP2326003B1/en active Active
- 2010-11-24 TW TW099140628A patent/TWI430576B/en active
Also Published As
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TW201141062A (en) | 2011-11-16 |
EP2326003A1 (en) | 2011-05-25 |
US7969189B2 (en) | 2011-06-28 |
US20110121859A1 (en) | 2011-05-26 |
EP2326003B1 (en) | 2017-01-04 |
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